2004
DOI: 10.1111/j.1365-2966.2004.07787.x
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Compton tails in long-duration gamma-ray bursts

Abstract: Some of the phenomena related to the prompt gamma‐ray burst emission could be interpreted as the presence of a consistent amount of material (Thomson optical depth ∼1) at rest and close to the source at a typical distance of ∼1015 cm. The material optical depth τ=σ〈n〉ΔR, where 〈n〉 is the average particle density over the distance ΔR, will attenuate the prompt gamma‐ray flux by an amount e−τ, while producing a secondary flux proportional to 1 − e−τ of scattered photons with a partly modified energy spectrum. Th… Show more

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Cited by 7 publications
(8 citation statements)
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“…Possibility (ii) postulates the existence of some scattering material along the line of sight, following the original idea of Brainerd (1994) and Brainerd et al (1998), and later used also by Barbiellini et al (2004). In this case we are receiving the transmitted flux piercing through the scattering screen.…”
Section: Introductionmentioning
confidence: 99%
“…Possibility (ii) postulates the existence of some scattering material along the line of sight, following the original idea of Brainerd (1994) and Brainerd et al (1998), and later used also by Barbiellini et al (2004). In this case we are receiving the transmitted flux piercing through the scattering screen.…”
Section: Introductionmentioning
confidence: 99%
“…[2] ascribed these bumps to the Compton scattering of the prompt gamma-ray photons on the circumburst material surrounding the burst progenitor. [2] assumed a shell of material with uniform density n and thickness R 0 located at distance R 0 from the central engine, which implies an optical depth to Compton scattering τ ∼ σ nR. Because of the Compton scattering the prompt gamma-ray photons are attenuated by a factor e −τ , and the resulting synchrotron flux is L s ∼ (n p e −τ )/(πθ 2 j t grb ), where n p is the number of gamma-ray photons, θ j is the burst jet aperture, and t grb is the burst duration.…”
Section: Motivation For An Alternative Grb Emission Mechanismmentioning
confidence: 99%
“…2 and the empirical relation implied by the Compton tail of the prompt emission, i.e. τR = σ T n 0 R 2 0 = const [2] to express the model parameters R 0 , n 0 and θ j in terms of only the measured quantities α p and T pro . This permit us to write GRB peak energy E p and its isotropic energy E iso in terms of only observed quantities (see [5] for details):…”
Section: Prediction: Grb Light Curves and Spectral-total Energy Corrementioning
confidence: 99%
“…In the astrophysical context of particle acceleration in GRBs, wakefield acceleration has been studied in the coherent regime where the forcing of the plasma is done by the electromagnetic field (Hoshino 2008;Liang & Noguchi 2007). Incoherent-or stochastic-wakefield processes have to our knowledge so far not been studied numerically, and have been considered theoretically only in a few cases (e.g., Barbiellini et al 2004Barbiellini et al , 2006.…”
Section: Introductionmentioning
confidence: 98%